2017
Publication Year
2020-07-24T13:52:29Z
Acceptance in OA@INAF
The Distinct Build-Up Of Dense And Normal Massive Passive Galaxies In Vipers
Title
GARGIULO, ADRIANA; Vipers Team
Authors
10.5281/zenodo.807380
DOI
http://hdl.handle.net/20.500.12386/26631
The distinct build up of
dense and normal
passive galaxies in VIPERS
ADRIANA GARGIULO & THE VIPERS TEAM
• Why studying massive (Mstar > 1011M
sun) passive galaxies (MPGs)
• The evolution of the number density and of the stellar population ages of MPGs at 0.5 < z <1.0 • The impact of the environment on the mass assembly history of MPGs
Most of the stellar mass in galaxies today resides in massive passive systems
(e.g. Renzini 2006).
Still unclear WHEN & WHERE the stars in massive galaxies were formed
THE ‘MERGER’ (EX SITU) HYPOTHESIS
In a ΛCDM Universe the assembly of massive galaxies is dominated by the (dry) accretion
of stars formed in other galaxies
(e.g. Naab+ 2009; Qu+ 2017; Rodriguez-Gomez+ 2016; Gabor&Davè 2012; Lackner+ 2012 / e.g.
Robertson+ 2006; Cox+ 2006; Pipino+ 2008)
THE IN SITU HYPOTHESIS
Stars in massime galaxies come from in situ star formation (untill an event – e.g.
AGN feedback, halo shock, disc fragmantation – does not stop it)
(Genzel+ 2008, 2011; Förster Schreiber+ 2011; Tacconi+ 2013; Wuyts+ 2013)
STRUCTURAL PROPERTIES OF LOCAL AND HIGH-Z MPGs
THE EX SITU HYPOTHESIS vs. THE IN SITU HYPOTHESIS Do we need a combination of these?
Evolutionary models have to reproduce MPGs properties as the size-mass relation and its evolution with time
Belli et al. 2014
At fixed stellar mass
• local MPGs have dimensions that vary up to an order of magnitude;
• high-z (z ~ 2) MPGs are smaller than local MPGs by a factor ~ 5
STRUCTURAL PROPERTIES OF LOCAL AND HIGH-Z MPGs
THE EX SITU HYPOTHESIS vs. THE IN SITU HYPOTHESIS Do we need a combination of these?
Evolutionary models have to reproduce MPGs properties as the size-mass relation and its evolution with time
Given the mean stellar mass density Σ = M* /(2 π Re2)
on average
high – z MPGs were denser than local MPGs
THE OPEN QUESTIONS
• Why, at fixed stellar mass, the typical dimension of a MPGs varies up to an order of magnitude?
• Have dense and less dense local MPGs different stellar mass assembly history?
In which way was build up the population of local MPGs?
TO FIND THE ANSWER WE STUDIED:
1. the evolution of the number density of MPGs as a function of Σ
2. the evolution of the stellar population ages of MPGs as a function of Σ 3. the correlation of Σ and the local environment
VIMOS PUBLIC EXTRAGALACTIC REDSHIFT SURVEY
VIPERS IN A NUTSHELL
ESO LARGE PROGRAM (PI: L. Guzzo) SPECTRA :
LRR grism (R = 200) [5500 – 9500] A Δz = 0.00047(1 + z) TARGET SAMPLE :
• i(AB) < 22.5 on the CFHTLS Wide W1 and W4 fields • ugri colour pre-selection z > 0.5
VOLUME :
5 x 107 h-3 Mpc3 - comparable to 2DF but at redshift ~ 1
AREA :
24 sq. dg (~ 16 without gaps) – 40% sampling rate PHOTOMETRY : NUV, u, g, r, i, z, K ++ (Moutard et al. 2016)
Now available at
http://vipers.inaf.it/
THE VIPERS SAMPLE OF MPGs
The selection criteria:
•
2 ≤ zflag ≤ 9.0•
0.5 ≤ z ≤ 1.0•
(NUV – r) vs (r –K)•
Mstar ≥ 1011 Msun (Cha IMF)
~2000 MPGs at 0.5 < z < 1.0 with z-spec
To derive Σ: Re in i band for galaxies at z ≥ 0.8
Re r band for galaxies at z < 0.8 ~ U band rest frame over the whole redshift range
Davidzon et al. 2013, 2016
For structural parameters in VIPERS see Krywult+ 2016, δRe < 10%
High-Σ MPGs Σ > 2000Msun pc-2 --- Intermediate- Σ MPGs 1000 < Σ ≤ 2000M
sun pc-2 Low- Σ MPGs Σ ≤ 1000Msun pc-2
THE EVOLUTION OF THE NUMBER DENSITY OF MPGs
AS A FUNCTION OF Z AND Σ
Number densities fully corrected for incompleteness
Errors take into account the Poisson fluctuations and the error on Re The evolution of the number densities
depends on Σ :
the lower the Σ, the faster the evolution From z = 1.0 z = 0.5: Increase factor: Total : ~ 2.5 High Σ : ~ 1.2 Int Σ : ~ 1.7 Low Σ : ~ 4.2
THE EVOLUTION OF THE STELLAR POPULATION AGES OF MPGs
AS A FUNCTION OF Z AND Σ
Compact MPGs
The evolution both of the number density and of the mean age of dense MPGs show that they passively evolve
The approach:
1. ages derived from the SED fitting Mean Age/Z/Tau (z, Σ); 2. Mean Age/Z/Tau (z, Σ) + BC03 models D4000SED (z, Σ); 3. D4000SED (z, Σ) vs D4000obs(z, Σ)
MEAN AGE FROM SED
MEAN OBSERVED D4000n
MEAN SED D4000n
THE EVOLUTION OF THE STELLAR POPULATION AGES OF MPGs
AS A FUNCTION OF Z AND Σ
The evolution of the number density and of the mean age of less dense MPGs show that a significant fraction of NEW and YOUNGER MPGs should
appear at later epoch
Dense MPGs are older than less dense ones
(see also, e.g. , Poggianti+ 2013, Saracco+ 2010, Williams+ 2016, Fagioli+ 2016 at smaller Mstar) Less dense MPGs
CONCLUSIONS - 1
From redshift 1.0 to 0.5
the population of MPGs (mainly) grows bottom – up:
on top of the population of denser MPGs already in place at z ~ 1.0, new, younger, and larger MPGs appear at lower z
CONCLUSIONS - 1
From redshift 1.0 to 0.5
the population of MPGs (mainly) grows bottom – up:
on top of the population of denser MPGs already in place at z ~ 1.0, new, younger, and larger MPGs appear at lower z
The increase in number density of MPGs at z < 0.8 is totally accounted for by the
decrease in number density of active massive galaxies
Active massive galaxies most likely progenitors of MPGs
(see, e.g. Lilly & Carollo 2016).
THE PROGENITORS OF (LESS DENSE) MPGs
dry mergers
Increase in the number density
due to other MPGs formation channels, e.g. dry mergers
Any other channel of MPGs formation
different from the quenching of active massive galaxies will result in an overabundance
THE IMPACT OF THE ENVIRONMENT ON Σ
Dry mergers increase the galaxy size + merger activity enhanced in higher density regions
Larger galaxies in denser environment
δ = [ρ (ra, dec,z)/ρ (z) ] - 1
5° neigh.
2000 km/s
THE IMPACT OF THE STELLAR MASS DISTRIBUTION
ON THE δ vs. Σ CORRELATION
THE IMPACT OF THE STELLAR MASS DISTRIBUTION
ON THE δ vs. Σ CORRELATION
Positive corralation bewteen Mstar and Re& δ
Spurious positive correlation between δ and Σ
Mass-matched samples
(PRELIMINARY) RESULTS
At Mstar < 2*1011M
sun we do not find
significative evidence of a trend between δ and Σ
Low-Σ MPGs
High-Σ MPGs
(PRELIMINARY) RESULTS
Lack(abundance) of compact(less dense) verymassive PGs
in the densest regions:
1. High density regions
prevent(favor) the formation of compact(less dense) MPGs with
Mstar > 2*1011M sun
(PRELIMINARY) RESULTS
Lack(abundance) of compact(less dense) verymassive PGs
in the densest regions:
1. High density regions
prevent(favor) the formation of compact(less dense) MPGs with
Mstar > 2*1011M sun
2. Or compact MPGs with Mstar > 2*1011M
sun disappear from high- δ
regions ( less dense) t = to
(PRELIMINARY) RESULTS
Lack(abundance) of compact(less dense) verymassive PGs
in the densest regions:
1. High density regions
prevent(favor) the formation of compact(less dense) MPGs with
Mstar > 2*1011M sun
2. Or compact MPGs with Mstar > 2*1011M
sun disappear from high- δ
regions ( less dense) t = t1 > to
(PRELIMINARY) RESULTS
Δn
Δn
BCGs ‘creation’?
The drop in the number of compact MPGs in the highest desnity regions
=
to the increase in the number of less dense MPGs in the highest density
(PRELIMINARY) RESULTS
Δn
Δn
BCGs ‘creation’?
Thank you!
The drop in the number of compact MPGs in the highest desnity regions
=
to the increase in the number of less dense MPGs in the highest density